Divergent Fluctuations from a 2D Infrared Catastrophe

Fuente: arXiv
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Autores principales: Hennig, Richard G., Cucinotta, Clotilde S.
Formato: Preprint
Publicado: 2026
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author Hennig, Richard G.
Cucinotta, Clotilde S.
author_facet Hennig, Richard G.
Cucinotta, Clotilde S.
contents Molecular simulations of interfacial polar media routinely employ periodic boundary conditions parallel to the interface. We show that this lateral periodicity introduces a spatially uniform in-plane mode ($q_{\parallel}=0$) that is unscreened because every lateral replica carries identical charge fluctuations. This 2D mode reduces the plane-averaged potential to a stochastic integral of the plane-averaged charge density along $z$, so that in a semi-infinite slab the variance of the potential grows linearly with depth. In a finite or periodic cell along $z$, with boundaries held at fixed potential, it follows a parabolic profile--a Brownian bridge--pinned to zero at both ends, with amplitude inversely proportional to the lateral cell area. These diverging fluctuations are a pure artifact of the imposed 2D lateral periodicity: they remain bounded in systems that are non-periodic or of finite lateral extent. We provide an analytic expression for their magnitude in dipolar media, yielding a practical criterion for the choice of lateral cell dimensions.
format Preprint
id arxiv_https___arxiv_org_abs_2601_09009
institution arXiv
publishDate 2026
record_format arxiv
spellingShingle Divergent Fluctuations from a 2D Infrared Catastrophe
Hennig, Richard G.
Cucinotta, Clotilde S.
Statistical Mechanics
Materials Science
Computational Physics
Molecular simulations of interfacial polar media routinely employ periodic boundary conditions parallel to the interface. We show that this lateral periodicity introduces a spatially uniform in-plane mode ($q_{\parallel}=0$) that is unscreened because every lateral replica carries identical charge fluctuations. This 2D mode reduces the plane-averaged potential to a stochastic integral of the plane-averaged charge density along $z$, so that in a semi-infinite slab the variance of the potential grows linearly with depth. In a finite or periodic cell along $z$, with boundaries held at fixed potential, it follows a parabolic profile--a Brownian bridge--pinned to zero at both ends, with amplitude inversely proportional to the lateral cell area. These diverging fluctuations are a pure artifact of the imposed 2D lateral periodicity: they remain bounded in systems that are non-periodic or of finite lateral extent. We provide an analytic expression for their magnitude in dipolar media, yielding a practical criterion for the choice of lateral cell dimensions.
title Divergent Fluctuations from a 2D Infrared Catastrophe
topic Statistical Mechanics
Materials Science
Computational Physics
url https://arxiv.org/abs/2601.09009